CN109873163B - A current collector, its pole piece and battery and application - Google Patents
A current collector, its pole piece and battery and application Download PDFInfo
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- CN109873163B CN109873163B CN201711267487.XA CN201711267487A CN109873163B CN 109873163 B CN109873163 B CN 109873163B CN 201711267487 A CN201711267487 A CN 201711267487A CN 109873163 B CN109873163 B CN 109873163B
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- H01M4/02—Electrodes composed of, or comprising, active material
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- H01M10/052—Li-accumulators
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- H—ELECTRICITY
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- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M10/00—Secondary cells; Manufacture thereof
- H01M10/05—Accumulators with non-aqueous electrolyte
- H01M10/052—Li-accumulators
- H01M10/0525—Rocking-chair batteries, i.e. batteries with lithium insertion or intercalation in both electrodes; Lithium-ion batteries
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- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M10/00—Secondary cells; Manufacture thereof
- H01M10/42—Methods or arrangements for servicing or maintenance of secondary cells or secondary half-cells
- H01M10/4235—Safety or regulating additives or arrangements in electrodes, separators or electrolyte
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M10/00—Secondary cells; Manufacture thereof
- H01M10/42—Methods or arrangements for servicing or maintenance of secondary cells or secondary half-cells
- H01M10/48—Accumulators combined with arrangements for measuring, testing or indicating the condition of cells, e.g. the level or density of the electrolyte
- H01M10/486—Accumulators combined with arrangements for measuring, testing or indicating the condition of cells, e.g. the level or density of the electrolyte for measuring temperature
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- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M4/00—Electrodes
- H01M4/02—Electrodes composed of, or comprising, active material
- H01M4/64—Carriers or collectors
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
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- H01M4/00—Electrodes
- H01M4/02—Electrodes composed of, or comprising, active material
- H01M4/64—Carriers or collectors
- H01M4/66—Selection of materials
- H01M4/661—Metal or alloys, e.g. alloy coatings
- H01M4/662—Alloys
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M4/00—Electrodes
- H01M4/02—Electrodes composed of, or comprising, active material
- H01M4/64—Carriers or collectors
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- H01M4/664—Ceramic materials
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- H01M50/00—Constructional details or processes of manufacture of the non-active parts of electrochemical cells other than fuel cells, e.g. hybrid cells
- H01M50/50—Current conducting connections for cells or batteries
- H01M50/572—Means for preventing undesired use or discharge
- H01M50/574—Devices or arrangements for the interruption of current
- H01M50/581—Devices or arrangements for the interruption of current in response to temperature
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- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
- Y02E60/10—Energy storage using batteries
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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Abstract
本申请涉及电池领域,具体地讲,涉及一种集流体、其极片和电池及应用。本申请的集流体包括具有支撑作用的绝缘层和具有导电和集流作用的导电层,导电层的常温薄膜电阻RS满足:0.01Ω/□≤RS≤0.15Ω/□。该集流体可大大提高电池异常情况下发生短路时的短路电阻,使短路电流大幅度减小,因此可极大地降低短路产热量,极大地改善电池的安全性能;另外由于产热量小,因此在发生内短路的位点处产生的热量可以被电池完全吸收,对电池造成的温升也很小,从而可以将短路损坏对电池的影响局限于“点”范围,仅形成“点断路”,而不影响电池在短时间内的正常工作。
The present application relates to the field of batteries, in particular, to a current collector, its pole piece, batteries and applications. The current collector of the present application includes an insulating layer with supporting function and a conductive layer with conductive and current collecting functions, and the normal temperature sheet resistance R S of the conductive layer satisfies: 0.01Ω/□≦R S ≦0.15Ω/□. The current collector can greatly improve the short-circuit resistance when the battery is short-circuited under abnormal conditions, so that the short-circuit current can be greatly reduced, so it can greatly reduce the short-circuit heat generation and greatly improve the safety performance of the battery; The heat generated at the site where the internal short circuit occurs can be completely absorbed by the battery, and the temperature rise caused to the battery is also small, so that the impact of the short-circuit damage on the battery can be limited to the "point" range, and only a "point open circuit" is formed. It does not affect the normal operation of the battery in a short period of time.
Description
技术领域technical field
本申请涉及电池领域,具体地讲,涉及一种集流体,其极片和电池及应用。The present application relates to the field of batteries, in particular, to a current collector, its pole piece, batteries and applications.
背景技术Background technique
锂离子电池由于具备能量密度大、输出功率高、循环寿命长和环境污染小等优点而被广泛应用于电动汽车以及消费类电子产品中。然而锂离子电池在受到挤压、碰撞或穿刺等异常情况时很容易发生着火、爆炸,从而引起严重危害。因此锂离子电池的安全问题很大程度地限制了锂离子电池的应用和普及。Lithium-ion batteries are widely used in electric vehicles and consumer electronic products due to their advantages of high energy density, high output power, long cycle life and low environmental pollution. However, lithium-ion batteries are prone to fire and explode when subjected to abnormal conditions such as extrusion, collision or puncture, causing serious harm. Therefore, the safety problem of lithium-ion batteries limits the application and popularization of lithium-ion batteries to a great extent.
大量实验结果表明,电池内短路是造成锂离子电池安全隐患的根本所在。为了避免发生电池内短路,研究者们试图改进隔膜结构、电池机械结构等。其中有些研究是从改善集流体的设计方面来提升锂离子电池的安全性能。A large number of experimental results show that the short circuit in the battery is the root cause of the safety hazard of lithium-ion batteries. In order to avoid the occurrence of short circuit in the battery, researchers have tried to improve the structure of the separator and the mechanical structure of the battery. Some of these studies are aimed at improving the safety performance of lithium-ion batteries by improving the design of current collectors.
当由于发生碰撞、挤压、穿刺等异常情况而导致电池发生内短路时,电池温度会上升;已有技术中有采用在金属集流体的材料中加入低熔点合金的技术方案,随着电池温度的上升,该集流体中的低熔点合金发生熔融,从而造成极片断路,由此切断电流,从而改善了电池的安全性;或采用具有树脂层两面复合有金属层的多层结构的集流体,随着电池温度的上升,当达到树脂层的材料的熔点时,该集流体的树脂层熔融而使极片破损,由此切断电流,从而改善电池的安全问题。When an internal short circuit occurs in the battery due to abnormal conditions such as collision, extrusion, puncture, etc., the battery temperature will rise; in the prior art, there is a technical solution of adding a low melting point alloy to the material of the metal current collector. As the current rises, the low melting point alloy in the current collector is melted, causing the pole piece to open circuit, thereby cutting off the current, thereby improving the safety of the battery; or using a multi-layer structure current collector with a resin layer and a metal layer on both sides As the battery temperature rises, when the melting point of the resin layer material is reached, the resin layer of the current collector melts and the pole piece is damaged, thereby cutting off the current, thereby improving the safety of the battery.
然而已有技术中的这些方法都无法有效地阻止锂离子电池内短路的发生,而且也无法保证在异常情况发生后电池还可以继续工作。在上述这些改进方法中,电池发生内短路后,电池温度依然会急剧升高,当电池温度骤升时,若安全构件不能快速响应的话,则依然会发生不同程度的危险;而且在上述这些改进方法中,在安全构件响应后,虽然电池的安全隐患得以解决,然而电池却无法继续工作。However, none of these methods in the prior art can effectively prevent the occurrence of a short circuit in the lithium ion battery, and also cannot guarantee that the battery can continue to work after an abnormal situation occurs. In the above improved methods, the temperature of the battery will still rise sharply after the internal short circuit occurs in the battery. When the temperature of the battery rises sharply, if the safety component cannot respond quickly, there will still be dangers to varying degrees; and in the above improvements In the method, after the safety component responds, although the safety hazard of the battery is solved, the battery cannot continue to work.
因此,有必要提供一种能在碰撞、挤压、穿刺等异常情况发生后,有效地防止电池由于内短路的发生而引起的着火、爆炸等事故且不影响电池正常工作的集流体和电池设计。Therefore, it is necessary to provide a current collector and a battery design that can effectively prevent accidents such as fire and explosion caused by the occurrence of internal short circuits in the battery after collision, extrusion, puncture, etc., without affecting the normal operation of the battery. .
发明内容SUMMARY OF THE INVENTION
鉴于此,本申请提出一种集流体,其极片和电池及应用。In view of this, the present application proposes a current collector, its pole piece, battery and application.
第一方面,本申请提出一种集流体;包括绝缘层和导电层,所述绝缘层用于承载所述导电层;所述导电层用于承载电极活性材料层,且所述导电层位于所述绝缘层的至少一个表面上,所述导电层的常温薄膜电阻RS满足:0.01Ω/□≤RS≤0.15Ω/□。In a first aspect, the present application proposes a current collector; comprising an insulating layer and a conductive layer, the insulating layer is used for supporting the conductive layer; the conductive layer is used for supporting the electrode active material layer, and the conductive layer is located in the On at least one surface of the insulating layer, the normal temperature sheet resistance R S of the conductive layer satisfies: 0.01Ω/□≦R S ≦0.15Ω/□.
第二方面,本申请提出该集流体在制备受到引发短路的异常情况时仅形成点断路以自身保护的电池中的应用。In the second aspect, the present application proposes the application of the current collector in preparing a battery that only forms a point disconnection for self-protection when subjected to an abnormal situation that causes a short circuit.
第三方面,本申请提出该集流体作为受到引发短路的异常情况时仅形成点断路的电池的集流体的用途。In a third aspect, the present application proposes the use of the current collector as a current collector for a battery that only forms a point disconnection when subjected to an abnormal situation that causes a short circuit.
第四方面,本申请提出一种极片,包括第一方面的集流体。In a fourth aspect, the present application provides a pole piece including the current collector of the first aspect.
第五方面,本申请提出一种电池,包括第四方面的极片。In a fifth aspect, the present application provides a battery including the pole piece of the fourth aspect.
本申请的技术方案至少具有以下有益的效果:The technical solution of the present application has at least the following beneficial effects:
本申请提出一种集流体,该集流体包括具有支撑作用的绝缘层和具有导电和集流作用的导电层,导电层的常温薄膜电阻RS满足:0.01Ω/□≤RS≤0.15Ω/□。该集流体可大大提高电池异常情况下发生短路时的短路电阻,使短路电流大幅度减小,因此可极大地降低短路产热量,极大地改善电池的安全性能;另外由于产热量小,因此在发生内短路的位点处产生的热量可以被电池完全吸收,对电池造成的温升也很小,从而可以将短路损坏对电池的影响局限于“点”范围,仅形成“点断路”,而不影响电池在短时间内的正常工作。本申请的集流体的导电层还可以包括导电层本体和位于导电层本体的至少一个表面上的保护层,从而可以大大改善该集流体的工作稳定性和使用寿命。The present application proposes a current collector, the current collector includes an insulating layer with supporting function and a conductive layer with conductive and current collecting functions, and the normal temperature sheet resistance R S of the conductive layer satisfies: 0.01Ω/□≤R S ≤0.15Ω/ □. The current collector can greatly improve the short-circuit resistance when the battery is short-circuited under abnormal conditions, so that the short-circuit current can be greatly reduced, so it can greatly reduce the short-circuit heat generation and greatly improve the safety performance of the battery; The heat generated at the site where the internal short circuit occurs can be completely absorbed by the battery, and the temperature rise caused to the battery is also small, so that the impact of the short-circuit damage on the battery can be limited to the "point" range, and only a "point open circuit" is formed. It does not affect the normal operation of the battery in a short period of time. The conductive layer of the current collector of the present application may further include a conductive layer body and a protective layer on at least one surface of the conductive layer body, so that the working stability and service life of the current collector can be greatly improved.
并且,具有该集流体的电池可以同时或连续受到多次内短路损坏,均不会发生着火、爆炸等事故,且均可以在短时间内正常工作。此外,导电层的常温薄膜电阻处于上述范围的集流体既具有优异的安全性能,又可以使电池具有良好的放电容量、倍率性能等电化学性能。Moreover, the battery with the current collector can be damaged by multiple internal short circuits at the same time or in succession, all accidents such as fire and explosion will not occur, and all can work normally in a short period of time. In addition, the current collector with the normal temperature sheet resistance of the conductive layer in the above range not only has excellent safety performance, but also enables the battery to have good electrochemical performance such as discharge capacity and rate performance.
附图说明Description of drawings
图1为本申请某一具体实施方式的正极集流体的结构示意图;1 is a schematic structural diagram of a positive electrode current collector according to a specific embodiment of the present application;
图2为本申请又一具体实施方式的正极集流体的结构示意图;2 is a schematic structural diagram of a positive electrode current collector according to another specific embodiment of the present application;
图3为本申请某一具体实施方式的负极集流体的结构示意图;3 is a schematic structural diagram of a negative electrode current collector according to a specific embodiment of the present application;
图4为本申请又一具体实施方式的负极集流体的结构示意图;4 is a schematic structural diagram of a negative electrode current collector according to another specific embodiment of the present application;
图5为本申请又一具体实施方式的正极集流体的结构示意图;5 is a schematic structural diagram of a positive electrode current collector according to another specific embodiment of the present application;
图6为本申请又一具体实施方式的正极集流体的结构示意图;6 is a schematic structural diagram of a positive electrode current collector according to another specific embodiment of the present application;
图7为本申请又一具体实施方式的正极集流体的结构示意图;7 is a schematic structural diagram of a positive electrode current collector according to another specific embodiment of the present application;
图8为本申请又一具体实施方式的正极集流体的结构示意图;8 is a schematic structural diagram of a positive electrode current collector according to another specific embodiment of the present application;
图9为本申请又一具体实施方式的正极集流体的结构示意图;9 is a schematic structural diagram of a positive electrode current collector according to another specific embodiment of the present application;
图10为本申请又一具体实施方式的负极集流体的结构示意图;10 is a schematic structural diagram of a negative electrode current collector according to another specific embodiment of the present application;
图11为本申请又一具体实施方式的负极集流体的结构示意图;11 is a schematic structural diagram of a negative electrode current collector according to another specific embodiment of the present application;
图12为本申请又一具体实施方式的负极集流体的结构示意图;12 is a schematic structural diagram of a negative electrode current collector according to another specific embodiment of the present application;
图13为本申请又一具体实施方式的负极集流体的结构示意图;13 is a schematic structural diagram of a negative electrode current collector according to another specific embodiment of the present application;
图14为本申请又一具体实施方式的负极集流体的结构示意图;14 is a schematic structural diagram of a negative electrode current collector according to another specific embodiment of the present application;
图15为本申请又一具体实施方式的负极集流体的结构示意图;15 is a schematic structural diagram of a negative electrode current collector according to another specific embodiment of the present application;
图16为本申请又一具体实施方式的负极集流体的结构示意图;16 is a schematic structural diagram of a negative electrode current collector according to another specific embodiment of the present application;
图17为本申请某一具体实施方式的正极极片的结构示意图;17 is a schematic structural diagram of a positive electrode piece according to a specific embodiment of the present application;
图18为本申请又一具体实施方式的正极极片的结构示意图;18 is a schematic structural diagram of a positive electrode piece according to another specific embodiment of the present application;
图19为本申请某一具体实施方式的负极极片的结构示意图;19 is a schematic structural diagram of a negative pole piece according to a specific embodiment of the application;
图20为本申请又一具体实施方式的负极极片的结构示意图;20 is a schematic structural diagram of a negative pole piece according to another specific embodiment of the application;
图21为本申请一次穿钉实验示意图;Figure 21 is a schematic diagram of a nail penetration experiment of the application;
图22为电池1#和电池4#在一次穿钉实验后的温度变化曲线;Figure 22 is the temperature change curve of battery 1# and
图23为电池1#和电池4#在一次穿钉实验后的电压变化曲线;Figure 23 is the voltage change curve of battery 1# and
其中:in:
1-正极极片;1- positive pole piece;
10-正极集流体;10- positive current collector;
101-正极绝缘层;101- positive insulating layer;
102-正极导电层;102-anode conductive layer;
1021-正极导电层本体;1021- positive electrode conductive layer body;
1022-正极保护层;1022 - positive electrode protective layer;
11-正极活性材料层;11- positive electrode active material layer;
2-负极极片;2- negative pole piece;
20-负极集流体;20- negative electrode current collector;
201-负极绝缘层;201-negative insulating layer;
202-负极导电层;202- negative electrode conductive layer;
2021-负极导电层本体;2021-The body of the negative electrode conductive layer;
2022-负极保护层;2022-Anode protective layer;
21-负极活性材料层;21- negative electrode active material layer;
3-隔膜;3-diaphragm;
4-钉子。4- Nails.
具体实施方式Detailed ways
下面结合具体实施例,进一步阐述本申请。应理解,这些实施例仅用于说明本申请而不用于限制本申请的范围。The present application will be further described below with reference to specific embodiments. It should be understood that these examples are only used to illustrate the present application and not to limit the scope of the present application.
本申请实施例提供了一种集流体,包括绝缘层和导电层。绝缘层用于承载导电层,对导电层起到支撑和保护的作用;导电层用于承载电极活性材料层,用于为电极活性材料层提供电子,即起到导电和集流的作用;导电层位于绝缘层的至少一个表面上。Embodiments of the present application provide a current collector including an insulating layer and a conductive layer. The insulating layer is used to carry the conductive layer, which supports and protects the conductive layer; the conductive layer is used to carry the electrode active material layer, and is used to provide electrons for the electrode active material layer, that is, it plays the role of conduction and current collection; The layer is on at least one surface of the insulating layer.
图1和图2为本申请实施例正极集流体的结构示意图,如图1、图2所示,正极集流体10包括正极绝缘层101和正极导电层102,用于涂敷正极活性材料以制备正极极片。图3和图4为本申请实施例负极集流体的结构示意图,如图3、图4所示,负极集流体20包括负极绝缘层201和负极导电层202,用于涂敷负极活性材料以制备负极极片。其中,如图1和图3所示,可在绝缘层的相对的两个表面上均设置有导电层,如图2和图4所示,也可在仅绝缘层的一面上设置有导电层。FIG. 1 and FIG. 2 are schematic diagrams of the structure of the positive electrode current collector according to the embodiment of the present application. As shown in FIG. 1 and FIG. 2 , the positive electrode
下面对本申请实施例集流体的结构和性能进行详细描述。The structures and properties of the current collectors of the embodiments of the present application will be described in detail below.
[导电层][Conductive layer]
在本申请实施例的集流体中,导电层的常温薄膜电阻RS满足:0.01Ω/□≤RS≤0.15Ω/□。In the current collector of the embodiment of the present application, the sheet resistance R S of the conductive layer at room temperature satisfies: 0.01Ω/□≦R S ≦0.15Ω/□.
其中,导电层的薄膜电阻用欧姆/平方(Ω/□)来计量,可被应用于将导电体考虑为一个二维实体的二维系统,其与三维系统下所用的电阻率的概念对等。当使用到薄膜电阻这一概念的时候,电流理论上假设为沿着薄膜的平面流动。Among them, the sheet resistance of the conductive layer is measured in ohms/square (Ω/□), which can be applied to a two-dimensional system considering a conductor as a two-dimensional entity, which is equivalent to the concept of resistivity used in a three-dimensional system . When the concept of sheet resistance is used, current is theoretically assumed to flow along the plane of the film.
对于常规三维导体,电阻的计算公式为:For conventional three-dimensional conductors, the formula for calculating resistance is:
其中,ρ代表电阻率,A代表截面面积,L代表长度。截面面积可被分解为宽度W和薄膜厚度t,即,电阻可被记为:Among them, ρ is the resistivity, A is the cross-sectional area, and L is the length. The cross-sectional area can be decomposed into the width W and the film thickness t, that is, the resistance can be written as:
其中,RS即为薄膜电阻。当膜片为正方形形状,L=W,所测得的电阻R即为膜片的薄膜电阻RS,而且RS与L或W的大小无关,RS是单位正方形的电阻值,因此RS的单位可以表示为欧姆每平方(Ω/□)。Among them, R S is the thin film resistance. When the diaphragm is square, L=W, the measured resistance R is the sheet resistance R S of the diaphragm, and R S has nothing to do with the size of L or W, R S is the resistance value of the unit square, so R S The unit can be expressed as ohms per square (Ω/□).
本申请实施例的常温薄膜电阻是指在常温条件下对导电层采用四探针法测量得到的电阻值,其中常温指15℃~25℃。The room temperature thin film resistance in the embodiments of the present application refers to the resistance value measured by the four-probe method on the conductive layer under normal temperature conditions, wherein the normal temperature refers to 15°C to 25°C.
在现有的锂离子电池中,当在异常情况下发生电池内短路时,瞬间产生大电流,并伴随着大量的短路产热,这些热量通常还会引发正极铝箔集流体处的铝热反应,进而使电池发生着火、爆炸等。在本申请实施例中,通过提高集流体的常温薄膜电阻RS从而解决了上述技术问题。In the existing lithium-ion battery, when a short circuit occurs in the battery under abnormal conditions, a large current is generated instantaneously, and a large amount of short circuit heat is generated. This can cause the battery to catch fire or explode. In the embodiments of the present application, the above-mentioned technical problems are solved by increasing the normal temperature sheet resistance R S of the current collector.
电池的内阻通常包括电池欧姆内阻和电池极化内阻,其中活性物质电阻、集流体电阻、界面电阻、电解液组成等均会对电池内阻产生较明显的影响。The internal resistance of the battery usually includes the battery ohmic internal resistance and the battery polarization internal resistance, among which the active material resistance, current collector resistance, interface resistance, and electrolyte composition will all have a significant impact on the internal resistance of the battery.
在异常情况下发生短路时,由于发生内短路,电池的内阻会大大降低。因此增大集流体的电阻,可增大电池短路后的内阻,由此改善电池的安全性能。在本申请实施例中,当电池可将短路损坏对电池的影响局限于“点”范围,即可将短路损坏对电池的影响局限于损坏点位处,且由于集流体的高电阻使得短路电流大幅度减小,短路产热使电池的温升不明显,不影响电池在短时间内正常使用的特点,称为“点断路”。When a short circuit occurs under abnormal conditions, the internal resistance of the battery will be greatly reduced due to the occurrence of an internal short circuit. Therefore, increasing the resistance of the current collector can increase the internal resistance of the battery after short circuit, thereby improving the safety performance of the battery. In the embodiment of the present application, when the battery can limit the impact of short-circuit damage on the battery to the "point" range, the impact of short-circuit damage on the battery can be limited to the damage point, and the high resistance of the current collector makes the short-circuit current It is greatly reduced, and the short-circuit heat generation makes the temperature rise of the battery not obvious, and does not affect the normal use of the battery in a short period of time, which is called "point circuit breaker".
当导电层的常温薄膜电阻RS满足:0.01Ω/□≤RS≤0.15Ω/□时,可以使电池在发生内短路的情况下,短路电流大幅减小,因此可极大地降低短路产热量,极大地改善电池的安全性能;此外,还可将短路产热量控制在电池可以完全吸收的范围,因此在发生内短路的位点处产生的热量可以被电池完全吸收,对电池造成的温升也很小,从而可以将短路损坏对电池的影响局限于“点”范围,仅形成“点断路”,而不影响电池在短时间内的正常工作。When the sheet resistance R S of the conductive layer at room temperature satisfies: 0.01Ω/□≤R S ≤0.15Ω/□, the short-circuit current can be greatly reduced in the case of an internal short circuit of the battery, so the short-circuit heat generation can be greatly reduced , greatly improving the safety performance of the battery; in addition, the short-circuit heat generation can also be controlled within the range that the battery can fully absorb, so the heat generated at the site where the internal short-circuit occurs can be completely absorbed by the battery. It is also very small, so that the impact of short-circuit damage on the battery can be limited to the "point" range, and only a "point open circuit" is formed, without affecting the normal operation of the battery in a short period of time.
可选的,导电层的常温薄膜电阻RS满足:0.02Ω/□≤RS≤0.1Ω/□。Optionally, the normal temperature sheet resistance R S of the conductive layer satisfies: 0.02Ω/□≤R S ≤0.1Ω/□.
当导电层的常温薄膜电阻RS太大时,会影响导电层的导电和集流的作用,电子无法在集流体、电极活性材料层以及两者的界面之间进行有效地传导,即会增大导电层表面的电极活性材料层的极化,影响电池的放电容量、倍率性能等电化学性能。因此导电层的常温薄膜电阻RS满足:0.01Ω/□≤RS≤0.15Ω/□。When the normal temperature sheet resistance R S of the conductive layer is too large, it will affect the conduction and current collection functions of the conductive layer, and electrons cannot be effectively conducted between the current collector, the electrode active material layer and the interface between the two, that is, the increase in The polarization of the electrode active material layer on the surface of the large conductive layer affects the electrochemical performance of the battery such as discharge capacity and rate performance. Therefore, the normal temperature sheet resistance R S of the conductive layer satisfies: 0.01Ω/□≦R S ≦0.15Ω/□.
在本申请中,常温薄膜电阻RS的上限可为0.15Ω/□、0.12Ω/□、0.1Ω/□、0.09Ω/□、0.08Ω/□、0.07Ω/□、0.05Ω/□,常温薄膜电阻RS的下限可为0.01Ω/□、0.02Ω/□、0.025Ω/□、0.03Ω/□、0.04Ω/□;常温薄膜电阻RS的范围可由上限或下限的任意数值组成。In this application, the upper limit of the sheet resistance R S at room temperature may be 0.15Ω/□, 0.12Ω/□, 0.1Ω/□, 0.09Ω/□, 0.08Ω/□, 0.07Ω/□, 0.05Ω/□, at room temperature The lower limit of the sheet resistance R S can be 0.01Ω/□, 0.02Ω/□, 0.025Ω/□, 0.03Ω/□, 0.04Ω/□; the range of the normal temperature sheet resistance R S can be composed of any value of the upper limit or the lower limit.
此外,导电层的厚度对根据本申请的集流体的工作可靠性和工作寿命也具有较大影响。In addition, the thickness of the conductive layer also has a great influence on the working reliability and working life of the current collector according to the present application.
优选的,在本申请实施例集流体中,导电层的厚度为D2,D2满足:300nm≤D2≤2μm。如果导电层太薄的话,虽然有益于增大集流体的常温薄膜电阻RS,却易在极片加工工艺等过程中发生破损;如果导电层太厚的话,则会影响电池的重量能量密度,且会不利于增大导电层的常温薄膜电阻RS。Preferably, in the current collector of the embodiment of the present application, the thickness of the conductive layer is D2, and D2 satisfies: 300nm≤D2≤2μm. If the conductive layer is too thin, although it is beneficial to increase the normal temperature sheet resistance R S of the current collector, it is easy to be damaged in the process of pole piece processing; if the conductive layer is too thick, it will affect the weight energy density of the battery. And it will be disadvantageous to increase the normal temperature sheet resistance R S of the conductive layer.
其中,导电层的厚度D2的上限可为2μm、1.8μm、1.5μm、1.2μm、1μm、900nm、800nm、700nm、600nm、500nm,导电层的厚度D2的下限可为300nm、350nm、400nm、450nm;导电层的厚度D2的范围可由上限或下限的任意数值组成。优选为500nm≤D2≤1.5μm。The upper limit of the thickness D2 of the conductive layer can be 2 μm, 1.8 μm, 1.5 μm, 1.2 μm, 1 μm, 900 nm, 800 nm, 700 nm, 600 nm, 500 nm, and the lower limit of the thickness D2 of the conductive layer can be 300 nm, 350 nm, 400 nm, 450 nm ; The range of the thickness D2 of the conductive layer can be composed of any numerical value of the upper limit or the lower limit. Preferably, 500 nm≤D2≤1.5 μm.
可选的,导电层的材料选自金属导电材料、碳基导电材料中的至少一种。其中,金属导电材料优选铝、铜、镍、钛、银、镍铜合金、铝锆合金中的至少一种;碳基导电材料优选石墨、乙炔黑、石墨烯、碳纳米管中的至少一种。Optionally, the material of the conductive layer is selected from at least one of metal conductive materials and carbon-based conductive materials. Among them, the metal conductive material is preferably at least one of aluminum, copper, nickel, titanium, silver, nickel-copper alloy, and aluminum-zirconium alloy; the carbon-based conductive material is preferably at least one of graphite, acetylene black, graphene, and carbon nanotubes. .
其中,导电层可通过机械辊轧、粘结、气相沉积法(vapor deposition)、化学镀(Electroless plating)中的至少一种形成于绝缘层上,气相沉积法优选物理气相沉积法(Physical Vapor Deposition,PVD);物理气相沉积法优选蒸发法、溅射法中的至少一种;蒸发法优选真空蒸镀法(vacuum evaporating)、热蒸发法(Thermal EvaporationDeposition)、电子束蒸发法(electron beam evaporation method,EBEM)中的至少一种,溅射法优选磁控溅射法(Magnetron sputtering)。The conductive layer can be formed on the insulating layer by at least one of mechanical rolling, bonding, vapor deposition, and electroless plating. The vapor deposition method is preferably physical vapor deposition. , PVD); physical vapor deposition method is preferably at least one of evaporation method and sputtering method; evaporation method is preferably vacuum evaporation method (vacuum evaporating), thermal evaporation method (Thermal Evaporation Deposition), electron beam evaporation method (electron beam evaporation method) , EBEM) at least one, the sputtering method is preferably a magnetron sputtering method (Magnetron sputtering).
进一步的,本申请实施例集流体的导电层可包括导电层本体和位于导电层本体至少一个表面上的保护层。保护层可以防止导电层本体被氧化、腐蚀或破坏,从而可以大大改善该集流体的工作稳定性和使用寿命。Further, the conductive layer of the current collector in the embodiment of the present application may include a conductive layer body and a protective layer located on at least one surface of the conductive layer body. The protective layer can prevent the body of the conductive layer from being oxidized, corroded or destroyed, thereby greatly improving the working stability and service life of the current collector.
图5至图12为本申请实施例设置有保护层的集流体的结构示意图。正极集流体的示意图如图5至图10所示。5 to 12 are schematic structural diagrams of a current collector provided with a protective layer according to an embodiment of the present application. The schematic diagrams of the positive electrode current collectors are shown in FIGS. 5 to 10 .
在图5中,正极集流体10包括正极绝缘层101和设置于正极绝缘层101相对的两个表面上的正极导电层102,正极导电层102包括正极导电层本体1021以及设置于正极导电层本体1021背离正极绝缘层101的面(即,正极导电层本体1021的上表面)上的正极保护层1022。In FIG. 5 , the positive electrode
在图6中,正极集流体10包括正极绝缘层101和设置于正极绝缘层101相对的两个表面上的正极导电层102,正极导电层102包括正极导电层本体1021以及设置于正极导电层本体1021的朝向正极绝缘层101的面(即,正极导电层本体1021的下表面)上的正极保护层1022。In FIG. 6 , the positive electrode
在图7中,正极集流体10包括正极绝缘层101和设置于正极绝缘层101相对的两个表面上的正极导电层102,正极导电层102包括正极导电层本体1021以及设置于正极导电层本体1021的相对两个表面(即,正极导电层本体1021的上表面和下表面)上的正极保护层1022。In FIG. 7 , the positive electrode
在图8中,正极集流体10包括正极绝缘层101和设置于正极绝缘层101一个表面上的正极导电层102,正极导电层102包括正极导电层本体1021以及设置于正极导电层本体1021的背离正极绝缘层101的面(即,正极导电层本体1021的上表面)上的正极保护层1022。In FIG. 8 , the positive electrode
在图9中,正极集流体10包括正极绝缘层101和设置于正极绝缘层101一个表面上的正极导电层102,正极导电层102包括正极导电层本体1021以及设置于正极导电层本体1021的朝向正极绝缘层101的一面(即,正极导电层本体1021的下表面)上的正极保护层1022。In FIG. 9 , the positive electrode
在图10中,正极集流体10包括正极绝缘层101和设置于正极绝缘层一个表面上的正极导电层102,正极导电层102包括正极导电层本体1021以及设置于正极导电层本体1021的相对两个表面(即,正极导电层本体1021的上表面和下表面)上的正极保护层1022。In FIG. 10 , the positive electrode
同样的,负极集流体的示意图如图11至图16所示。Likewise, schematic diagrams of the negative electrode current collectors are shown in FIGS. 11 to 16 .
在图11中,负极集流体20包括负极绝缘层201和设置于负极绝缘层201相对的两个表面上的负极导电层202,负极导电层202包括负极导电层本体2021以及设置于负极导电层本体2021的背离负极绝缘层201的面(即,负极导电层本体2021的上表面)上的负极保护层2022。In FIG. 11 , the negative electrode
在图12中,负极集流体20包括负极绝缘层201和设置于负极绝缘层201相对的两个表面上的负极导电层202,负极导电层202包括负极导电层本体2021以及设置于负极导电层本体2021的朝向负极绝缘层201的面(即,负极导电层本体2021的下表面)上的负极保护层2022。In FIG. 12 , the negative electrode
在图13中,负极集流体20包括负极绝缘层201和设置于负极绝缘层201相对的两个表面上的负极导电层202,负极导电层202包括负极导电层本体2021以及设置于负极导电层本体2021的相对两个表面(即,负极导电层本体2021的上表面和下表面)上的负极保护层2022。In FIG. 13 , the negative electrode
在图14中,负极集流体20包括负极绝缘层201和设置于负极绝缘层201一个表面上的负极导电层202,负极导电层202包括负极导电层本体2021以及设置于负极导电层本体2021的背离负极绝缘层201(即,负极导电层本体2021的上表面)的面上的负极保护层2022。In FIG. 14 , the negative electrode
在图15中,负极集流体20包括负极绝缘层201和设置于负极绝缘层201一个表面上的负极导电层202,负极导电层202包括负极导电层本体2021以及设置于负极导电层本体2021的朝向负极绝缘层201的面(即,负极导电层本体2021的下表面)上的负极保护层2022。In FIG. 15 , the negative electrode
在图16中,负极集流体20包括负极绝缘层201和设置于负极绝缘层201一个表面上的负极导电层202,负极导电层202包括负极导电层本体2021以及设置于负极导电层本体2021的相对两个表面(即,负极导电层本体2021的上表面和下表面)上的负极保护层2022。In FIG. 16 , the negative electrode
可选地,保护层位于导电层本体的下表面上,即位于导电层本体与绝缘层之间。位于该位置的保护层不仅可以保护导电层本体,从而改善集流体的寿命和工作可靠性,还可以具有如下优点:(1)与位于导电层本体的上表面的保护层相比,位于导电层本体的下表面的保护层与导电层本体之间的结合力更强,更能起到保护导电层本体的作用;(2)位于导电层本体的下表面的保护层可以更好地增强集流体的机械强度;(3)位于导电层本体的下表面的保护层可以构成完整的支撑结构来保护导电层本体。Optionally, the protective layer is located on the lower surface of the conductive layer body, that is, between the conductive layer body and the insulating layer. The protective layer located at this position can not only protect the conductive layer body, thereby improving the life and working reliability of the current collector, but also have the following advantages: (1) Compared with the protective layer located on the upper surface of the conductive layer body, the conductive layer is located in the conductive layer. The bonding force between the protective layer on the lower surface of the body and the body of the conductive layer is stronger, and can better protect the body of the conductive layer; (2) the protective layer on the lower surface of the body of the conductive layer can better enhance the current collector (3) The protective layer on the lower surface of the conductive layer body can form a complete supporting structure to protect the conductive layer body.
可选地,保护层位于导电层本体的相对的两个表面上,即导电层本体的上表面和下表面上,从而最大程度地改善该集流体的工作稳定性和使用寿命,以及改善电池的容量保持率、循环寿命等性能。Optionally, the protective layer is located on two opposite surfaces of the conductive layer body, that is, the upper surface and the lower surface of the conductive layer body, so as to maximize the working stability and service life of the current collector and improve the battery life. Capacity retention rate, cycle life and other performance.
其中,导电层本体的材料选自金属导电材料、碳基导电材料中的至少一种。所述金属导电材料可选自铝、铜、镍、钛、银、镍铜合金、铝锆合金中的至少一种,所述碳基导电材料可选自石墨、乙炔黑、石墨烯、碳纳米管中的至少一种。Wherein, the material of the conductive layer body is selected from at least one of metal conductive materials and carbon-based conductive materials. The metal conductive material can be selected from at least one of aluminum, copper, nickel, titanium, silver, nickel-copper alloy, and aluminum-zirconium alloy, and the carbon-based conductive material can be selected from graphite, acetylene black, graphene, carbon nanomaterials at least one of the tubes.
保护层的材料可选自金属、金属氧化物、导电碳中的至少一种。可选的,金属选自镍、铬、镍基合金(如镍铬合金)、铜基合金(如铜镍合金)中的至少一种;可选的,金属氧化物选自氧化铝、氧化钴、氧化铬、氧化镍中的至少一种;可选的,导电碳选自导电炭黑、碳纳米管、乙炔黑、石墨烯中的至少一种。The material of the protective layer can be selected from at least one of metals, metal oxides, and conductive carbon. Optionally, the metal is selected from at least one of nickel, chromium, nickel-based alloys (such as nickel-chromium alloys), and copper-based alloys (such as copper-nickel alloys); optionally, the metal oxides are selected from aluminum oxide, cobalt oxide , at least one of chromium oxide, and nickel oxide; optionally, the conductive carbon is selected from at least one of conductive carbon black, carbon nanotubes, acetylene black, and graphene.
其中,镍基合金是以纯镍为基体加入一种或几种其他元素所构成的合金。优选为镍铬合金,镍铬合金是金属镍和金属铬形成的合金,可选的,镍元素与铬元素的摩尔比为1:99~99:1。Among them, the nickel-based alloy is an alloy composed of pure nickel as the matrix and one or several other elements added. It is preferably a nickel-chromium alloy, and the nickel-chromium alloy is an alloy formed by metal nickel and metal chromium. Optionally, the molar ratio of nickel element to chromium element is 1:99-99:1.
铜基合金是以纯铜为基体加入一种或几种其他元素所构成的合金。优选为铜镍合金,可选的,在铜镍合金中,镍元素与铜元素的摩尔比为1:99~99:1。Copper-based alloys are alloys formed by adding one or several other elements to the base of pure copper. It is preferably a copper-nickel alloy. Optionally, in the copper-nickel alloy, the molar ratio of nickel element to copper element is 1:99-99:1.
位于导电层本体的两个相对的表面上的保护层的材料可相同或不同,厚度可相同或不同。The materials of the protective layers on the two opposite surfaces of the conductive layer body may be the same or different, and the thicknesses may be the same or different.
保护层的厚度为D3,当D3≤1/10D2时,保护层对导电层的常温薄膜电阻的影响可忽略。The thickness of the protective layer is D3, and when D3≤1/10D2, the influence of the protective layer on the normal temperature sheet resistance of the conductive layer can be ignored.
作为本申请实施例集流体的进一步改进,保护层的厚度为D3,D3满足:D3≤1/10D2且1nm≤D3≤200nm,即厚度满足小于等于D2厚度的1/10在1nm~200nm范围内。其中,保护层的厚度D3的上限可为200nm、180nm、150nm、120nm、100nm、80nm、60nm、55nm、50nm、45nm、40nm、30nm、20nm,保护层的厚度D3的下限可为1nm、2nm、5nm、8nm、10nm、12nm、15nm、18nm;保护层的厚度D3的范围可由上限或下限的任意数值组成。如果保护层太薄,则不足以起到保护导电层的作用;保护层太厚,则会降低电池的重量能量密度和体积能量密度。优选的,10nm≤D3≤50nm。As a further improvement of the current collector in the embodiment of the present application, the thickness of the protective layer is D3, and D3 satisfies: D3≤1/10D2 and 1nm≤D3≤200nm, that is, the thickness satisfies 1/10 or less of the thickness of D2 in the range of 1nm~200nm . Wherein, the upper limit of the thickness D3 of the protective layer can be 200nm, 180nm, 150nm, 120nm, 100nm, 80nm, 60nm, 55nm, 50nm, 45nm, 40nm, 30nm, 20nm, and the lower limit of the thickness D3 of the protective layer can be 1nm, 2nm, 5nm, 8nm, 10nm, 12nm, 15nm, 18nm; the range of the thickness D3 of the protective layer can be composed of any numerical value of the upper limit or the lower limit. If the protective layer is too thin, it will not be enough to protect the conductive layer; if the protective layer is too thick, the weight energy density and volume energy density of the battery will be reduced. Preferably, 10nm≤D3≤50nm.
从保护层占整个导电层的厚度来看,优选的,D3满足:1/2000D2≤D3≤1/10D2,即厚度是D2的1/2000~1/10。更优选的,D3满足:1/1000D2≤D3≤1/10D2。From the perspective of the thickness of the protective layer accounting for the entire conductive layer, preferably, D3 satisfies: 1/2000D2≤D3≤1/10D2, that is, the thickness is 1/2000-1/10 of D2. More preferably, D3 satisfies: 1/1000D2≤D3≤1/10D2.
保护层可通过气相沉积法、原位形成法、涂布法等形成于导电层本体上。气相沉积法优选物理气相沉积法(Physical Vapor Deposition,PVD);物理气相沉积法优选蒸发法、溅射法中的至少一种;蒸发法优选真空蒸镀法(vacuum evaporating)、热蒸发法(ThermalEvaporation Deposition)、电子束蒸发法(electron beam evaporation method,EBEM)中的至少一种,溅射法优选磁控溅射法(Magnetron sputtering)。原位形成法优选原位钝化法,即在金属表面原位形成金属氧化物钝化层的方法。涂布法优选辊压涂布、挤压涂布、刮刀涂布、凹版涂布等中的一种。The protective layer may be formed on the conductive layer body by a vapor deposition method, an in-situ formation method, a coating method, or the like. The vapor deposition method is preferably a physical vapor deposition method (Physical Vapor Deposition, PVD); the physical vapor deposition method is preferably at least one of an evaporation method and a sputtering method; At least one of Deposition) and electron beam evaporation method (electron beam evaporation method, EBEM), the sputtering method is preferably magnetron sputtering (Magnetron sputtering). The in-situ formation method is preferably an in-situ passivation method, that is, a method in which a metal oxide passivation layer is formed in-situ on a metal surface. The coating method is preferably one of roll coating, extrusion coating, blade coating, gravure coating, and the like.
[绝缘层][Insulation]
在本申请实施例的集流体中,绝缘层主要起到支撑和保护导电层的作用,其厚度为D1,D1满足1μm≤D1≤20μm。若绝缘层太薄的话,很容易在极片加工工艺等过程中发生断裂;太厚的话,则会降低使用该集流体的电池的体积能量密度。In the current collector of the embodiment of the present application, the insulating layer mainly plays the role of supporting and protecting the conductive layer, and its thickness is D1, and D1 satisfies 1 μm≤D1≤20 μm. If the insulating layer is too thin, it is easy to break during the pole piece processing process, etc.; if it is too thick, it will reduce the volume energy density of the battery using the current collector.
其中,绝缘层的厚度D1的上限可为20μm、15μm、12μm、10μm、8μm,导电层的厚度D1的下限可为1μm、1.5μm、2μm、3μm、4μm、5μm、6μm、7μm;绝缘层的厚度D1的范围可由上限或下限的任意数值组成。优选为2μm≤D1≤10μm,更优选为2μm≤D1≤6μm。Wherein, the upper limit of the thickness D1 of the insulating layer can be 20 μm, 15 μm, 12 μm, 10 μm, 8 μm, and the lower limit of the thickness D1 of the conductive layer can be 1 μm, 1.5 μm, 2 μm, 3 μm, 4 μm, 5 μm, 6 μm, 7 μm; The range of the thickness D1 may be composed of any numerical value of the upper limit or the lower limit. Preferably, 2 μm≦D1≦10 μm, and more preferably 2 μm≦D1≦6 μm.
可选的,绝缘层的材料选自有机聚合物绝缘材料、无机绝缘材料、复合材料中的一种。进一步优选的,复合材料由有机聚合物绝缘材料和无机绝缘材料组成。Optionally, the material of the insulating layer is selected from one of organic polymer insulating materials, inorganic insulating materials, and composite materials. Further preferably, the composite material is composed of an organic polymer insulating material and an inorganic insulating material.
其中,有机聚合物绝缘材料选自聚酰胺(Polyamide,简称PA)、聚对苯二甲酸酯(Polyethylene terephthalate,简称PET)、聚酰亚胺(Polyimide,简称PI)、聚乙烯(Polyethylene,简称PE)、聚丙烯(Polypropylene,简称PP)、聚苯乙烯(Polystyrene,简称PS)、聚氯乙烯(Polyvinyl chloride,简称PVC)、丙烯腈-丁二烯-苯乙烯共聚物(Acrylonitrile butadiene styrene copolymers,简称ABS)、聚对苯二甲酸丁二醇酯(Polybutylene terephthalat,简称PBT)、聚对苯二甲酰对苯二胺(Poly-p-phenyleneterephthamide,简称PPA)、环氧树脂(epoxy resin)、聚丙乙烯(简称PPE)、聚甲醛(Polyformaldehyde,简称POM)、酚醛树脂(Phenol-formaldehyde resin)、聚四氟乙烯(Polytetrafluoroethylene,简称PTFE)、硅橡胶(Silicone rubber)、聚偏氟乙烯(Polyvinylidenefluoride,简称PVDF)、聚碳酸酯(Polycarbonate,简称PC)中的至少一种。The organic polymer insulating material is selected from polyamide (Polyamide, referred to as PA), polyethylene terephthalate (Polyethylene terephthalate, referred to as PET), polyimide (Polyimide, referred to as PI), polyethylene (Polyethylene, referred to as PI) PE), Polypropylene (PP), Polystyrene (PS), Polyvinyl chloride (PVC), Acrylonitrile butadiene styrene copolymers, Abbreviated as ABS), polybutylene terephthalate (Polybutylene terephthalat, referred to as PBT), poly-p-phenyleneterephthamide (Poly-p-phenyleneterephthamide, referred to as PPA), epoxy resin (epoxy resin), Polypropylene (PPE for short), Polyformaldehyde (POM), Phenol-formaldehyde resin, Polytetrafluoroethylene (PTFE), Silicone rubber, Polyvinylidenefluoride, At least one of PVDF for short) and Polycarbonate (PC for short).
无机绝缘材料优选氧化铝(Al2O3)、碳化硅(SiC)、二氧化硅(SiO2)中的至少一种;The inorganic insulating material is preferably at least one of aluminum oxide (Al 2 O 3 ), silicon carbide (SiC), and silicon dioxide (SiO 2 );
复合物优选环氧树脂玻璃纤维增强复合材料、聚酯树脂玻璃纤维增强复合材料中的至少一种。The composite is preferably at least one of epoxy resin glass fiber reinforced composite material and polyester resin glass fiber reinforced composite material.
由于绝缘层的密度通常较金属小,因此本申请集流体,在提升电池安全性能的同时,还可以提升电池的重量能量密度。并且由于绝缘层可以对位于其表面的导电层起到良好的承载和保护作用,因而不易产生传统集流体中常见的极片断裂现象。Since the density of the insulating layer is generally smaller than that of the metal, the current collector of the present application can improve the safety performance of the battery while also improving the weight energy density of the battery. And because the insulating layer can have a good bearing and protection effect on the conductive layer located on its surface, it is not easy to produce the phenomenon of pole piece fracture common in traditional current collectors.
本申请实施例的第二方面提供一种极片,包括本申请实施例第一方面的集流体和形成于集流体表面的电极活性材料层。A second aspect of the embodiments of the present application provides a pole piece including the current collector of the first aspect of the embodiments of the present application and an electrode active material layer formed on the surface of the current collector.
图17和图18为本申请实施例正极极片结构示意图,如图17和图18所示,正极极片1包括本申请的正极集流体10和形成于正极集流体10表面的正极活性材料层11,正极集流体10包括正极绝缘层101和正极导电层102。17 and 18 are schematic diagrams of the structure of the positive electrode sheet according to the embodiment of the present application. As shown in FIGS. 17 and 18 , the positive electrode sheet 1 includes the positive electrode
图19和图20为本申请实施例负极极片结构示意图,如图19和图20所示,负极极片2包括本申请的负极集流体20和形成于负极集流体20表面的负极活性材料层21,负极集流体20包括负极绝缘层201和负极导电层202。19 and FIG. 20 are schematic views of the structure of the negative electrode pole piece according to the embodiment of the present application. As shown in FIG. 19 and FIG. 20 , the negative
其中,当绝缘层的双面设置有导电层,集流体双面涂覆活性物质,制备得到的正极极片和负极极片分别如图17和图19所示,可直接应用于电池中。当绝缘层的单面设置有导电层时,集流体单面涂覆活性物质,制备得到的正极极片和负极极片分别如图18和图20所示,可折叠后应用于电池中。Among them, when the insulating layer is provided with a conductive layer on both sides, and the current collector is coated with active material on both sides, the prepared positive electrode and negative electrode are shown in Figure 17 and Figure 19 respectively, which can be directly used in batteries. When a conductive layer is provided on one side of the insulating layer, the active material is coated on one side of the current collector, and the prepared positive electrode and negative electrode are shown in Figure 18 and Figure 20, respectively, which can be folded and used in batteries.
本申请实施例的第三方面提供一种电池,包括正极极片、隔膜、负极极片和电解液。A third aspect of the embodiments of the present application provides a battery including a positive electrode sheet, a separator, a negative electrode sheet and an electrolyte.
其中,正极极片和/或负极极片为上述本申请实施例的极片。本申请的电池可为卷绕式,也可为叠片式。本申请的电池可以为锂离子二次电池、锂一次电池、钠离子电池、镁离子电池中的一种。但并不局限于此。Wherein, the positive pole piece and/or the negative pole piece are the pole pieces of the above embodiments of the present application. The battery of the present application may be of a wound type or a laminated type. The battery of the present application may be one of a lithium ion secondary battery, a lithium primary battery, a sodium ion battery, and a magnesium ion battery. But not limited to this.
进一步的,本申请实施例还提供一种电池,包括正极极片、隔膜、负极极片和电解液,仅正极极片为上述实施例中的正极极片。Further, an embodiment of the present application further provides a battery, including a positive electrode piece, a separator, a negative electrode piece and an electrolyte, and only the positive electrode piece is the positive electrode piece in the above embodiment.
优选地,本申请实施例电池的正极极片采用上述本申请的极片。因为常规正极集流体中的铝含量高,在电池异常情况下发生短路时,短路点处产生的热量可以引发剧烈的铝热反应,从而产生大量的热并引起电池发生爆炸等事故,所以当电池的正极极片采用本申请的极片时,由于正极集流体中铝的量大大减少,因此可以避免产生铝热反应,从而显著改善电池的安全性能。Preferably, the positive pole piece of the battery of the embodiment of the present application adopts the above-mentioned pole piece of the present application. Because the aluminum content in the conventional positive electrode current collector is high, when a short circuit occurs in the abnormal condition of the battery, the heat generated at the short circuit point can cause a violent aluminothermic reaction, thereby generating a large amount of heat and causing accidents such as battery explosion. When the positive electrode plate of the present application is used, since the amount of aluminum in the positive electrode current collector is greatly reduced, the aluminothermic reaction can be avoided, thereby significantly improving the safety performance of the battery.
下面通过采用穿钉实验来模拟电池的异常情况,以观察穿钉后电池的变化。图21为本申请实施例的电池发生一次穿钉实验示意图。为了简单起见,图中仅仅示出了钉子4穿透电池的一层正极极片1、一层隔膜3和一层负极极片2的情况。需要说明的是,实际的穿钉实验是钉子4穿透整个电池,通常包括多层正极极片1、多层隔膜3和多层负极极片2。根据图21可知,当电池因穿钉发生短路后,短路电流大幅减小,将短路产热量控制在电池可以完全吸收的范围,因此在发生内短路的位点处产生的热量可以被电池完全吸收,对电池造成的温升也很小,从而可以将短路损坏对电池的影响局限于穿钉位点,仅形成“点断路”,而不影响电池在短时间内的正常工作。Next, the abnormal condition of the battery is simulated by using the nail penetration experiment to observe the changes of the battery after nail penetration. FIG. 21 is a schematic diagram of a battery piercing experiment once in an embodiment of the present application. For the sake of simplicity, the figure only shows the situation where the
此外,本申请通过大量的实验发现,电池的容量越大,则电池的内阻越小,则电池的安全性能就越差,即电池容量(Cap)与电池内阻(r)呈反比关系:In addition, this application has found through a large number of experiments that the larger the capacity of the battery, the smaller the internal resistance of the battery, the worse the safety performance of the battery, that is, the battery capacity (Cap) and the battery internal resistance (r) are inversely proportional:
r=A/Capr=A/Cap
式中r表示电池的内阻,Cap表示电池的容量,A为系数。In the formula, r represents the internal resistance of the battery, Cap represents the capacity of the battery, and A is the coefficient.
电池容量Cap为电池的理论容量,通常为电池正极极片的理论容量。The battery capacity Cap is the theoretical capacity of the battery, usually the theoretical capacity of the positive electrode plate of the battery.
r可以通过内阻仪测试得到。r can be obtained through the internal resistance test.
对于由常规正极极片和常规负极极片组成的常规锂离子二次电池来说,由于在异常情况下发生内短路时,基本所有的常规锂离子二次电池均会发生不同程度的冒烟、起火、爆炸等。For conventional lithium-ion secondary batteries composed of conventional positive electrode and conventional negative electrode, due to the occurrence of internal short-circuit under abnormal conditions, almost all conventional lithium-ion secondary batteries will experience varying degrees of smoke, Fire, explosion, etc.
而对于本申请实施例的电池来说,由于在电池容量相同的情况下,具有比较大的电池内阻,因此可以具有较大的A值。However, for the battery of the embodiment of the present application, since the battery has a relatively large internal resistance under the condition of the same battery capacity, it can have a relatively large A value.
对于本申请实施例的电池来说,当系数A满足25Ah·mΩ≤A≤400Ah·mΩ时,电池可以兼具良好的电化学性能和良好的安全性能。For the batteries of the embodiments of the present application, when the coefficient A satisfies 25Ah·mΩ≤A≤400Ah·mΩ, the batteries can have both good electrochemical performance and good safety performance.
当A值太大时,电池由于内阻过大,电化学性能会劣化,因此没有实用性。When the A value is too large, the electrochemical performance of the battery will be deteriorated due to excessive internal resistance, so it is not practical.
当A值太小时,电池发生内短路时温升过高,电池安全性能降低。When the A value is too small, the temperature rise of the battery is too high when an internal short circuit occurs, and the safety performance of the battery is reduced.
进一步优选的,系数A满足30Ah·mΩ≤A≤200Ah·mΩ;更优选的,系数A满足40Ah·mΩ≤A≤150Ah·mΩ。More preferably, the coefficient A satisfies 30Ah·mΩ≤A≤200Ah·mΩ; more preferably, the coefficient A satisfies 40Ah·mΩ≤A≤150Ah·mΩ.
本申请实施例还涉及该集流体在制备受到引发短路的异常情况时仅形成点断路以自身保护的电池中的应用。在本申请中,当电池可将短路损坏对电池的影响局限于“点”范围,不影响电池在短时间内正常使用的特点,称为“点断路”。The embodiments of the present application also relate to the application of the current collector in preparing a battery that only forms a point disconnection for self-protection when subjected to an abnormal situation that causes a short circuit. In this application, when the battery can limit the impact of short-circuit damage on the battery to the "point" range, and does not affect the normal use of the battery in a short period of time, it is called "point open circuit".
另一方面,本申请实施例还涉及该集流体作为受到引发短路的异常情况时仅形成点断路的电池的集流体的用途。On the other hand, the embodiments of the present application also relate to the use of the current collector as a current collector of a battery that only forms a point disconnection when subjected to an abnormal condition that causes a short circuit.
优选的,引发短路的异常情况包括撞击、挤压、异物刺入等,由于在这些损伤过程中引发短路的均由具备一定导电性的材料将正负极电连接而引发,因此在本申请中将这些异常情况统称为穿钉。并在本申请具体实施方式中通过穿钉实验来模拟电池的异常情况。Preferably, the abnormal conditions that cause the short circuit include impact, extrusion, foreign object piercing, etc. Since the short circuit caused by these damage processes is caused by the electrical connection of the positive and negative electrodes with materials with certain conductivity, so in this application These abnormal conditions are collectively referred to as piercing. And in the specific embodiment of the present application, the abnormal situation of the battery is simulated through the nail penetration experiment.
实施例Example
1、集流体的制备:1. Preparation of current collector:
选取一定厚度的绝缘层,在其表面通过真空蒸镀、机械辊轧或粘结的方式形成一定厚度的导电层,并对导电层的常温薄膜电阻进行测定。Select an insulating layer of a certain thickness, form a conductive layer of a certain thickness on its surface by vacuum evaporation, mechanical rolling or bonding, and measure the normal temperature sheet resistance of the conductive layer.
其中,in,
(1)真空蒸镀方式的形成条件如下:将经过表面清洁处理的绝缘层置于真空镀室内,以1600℃至2000℃的高温将金属蒸发室内的高纯金属丝熔化蒸发,蒸发后的金属经过真空镀室内的冷却系统,最后沉积于绝缘层的表面,形成导电层。(1) The formation conditions of the vacuum evaporation method are as follows: place the insulating layer after surface cleaning treatment in the vacuum plating chamber, melt and evaporate the high-purity metal wire in the metal evaporation chamber at a high temperature of 1600 ℃ to 2000 ℃, and the evaporated metal After passing through the cooling system in the vacuum plating chamber, it is finally deposited on the surface of the insulating layer to form a conductive layer.
(2)机械辊轧方式的形成条件如下:将导电层材料的箔片置于机械辊中,通过施加20t至40t的压力将其碾压为预定的厚度,然后将其置于经过表面清洁处理的绝缘层的表面,最后将两者置于机械辊中,通过施加30t至50t的压力使两者紧密结合。(2) The forming conditions of the mechanical rolling method are as follows: the foil of the conductive layer material is placed in a mechanical roller, rolled to a predetermined thickness by applying a pressure of 20t to 40t, and then placed in a surface cleaning treatment The surface of the insulating layer is finally placed in a mechanical roller, and the two are tightly combined by applying a pressure of 30t to 50t.
(3)粘结方式的形成条件如下:将导电层材料的箔片置于机械辊中,通过施加20t至40t的压力将其碾压为预定的厚度;然后在经过表面清洁处理的绝缘层的表面涂布PVDF与NMP的混合溶液;最后将上述预定厚度的导电层粘结于绝缘层的表面,并于100℃下烘干。(3) The forming conditions of the bonding method are as follows: the foil of the conductive layer material is placed in a mechanical roller, and it is rolled to a predetermined thickness by applying a pressure of 20t to 40t; The surface is coated with a mixed solution of PVDF and NMP; finally, the above-mentioned conductive layer with a predetermined thickness is bonded to the surface of the insulating layer, and dried at 100°C.
(4)常温薄膜电阻测定方法为:(4) The method for measuring thin film resistance at room temperature is:
使用RTS-9型双电测四探针测试仪,测试环境为:常温23±2℃,相对湿度≤65%。测试时,将待测材料进行表面清洁,然后水平置于测试台上,将四探针放下,使探针与待测材料表面有良好接触,然后调节自动测试模式标定材料的电流量程,在合适的电流量程下进行薄膜方阻测量,并采集相同样品的8至10个数据点作为数据测量准确性和误差分析。Use RTS-9 double-electrical four-probe tester, the test environment is: normal temperature 23 ± 2 ℃, relative humidity ≤ 65%. During the test, clean the surface of the material to be tested, then place it horizontally on the test bench, put down the four probes to make the probes have good contact with the surface of the material to be tested, and then adjust the current range of the material to be calibrated in the automatic test mode. The thin-film square resistance measurement was carried out under the current range of 100, and 8 to 10 data points of the same sample were collected as the data measurement accuracy and error analysis.
本申请实施例和对比例的集流体及其极片具体参数如表1所示。The specific parameters of the current collectors and their pole pieces of the examples and comparative examples of the present application are shown in Table 1.
2、具有保护层的集流体的制备:2. Preparation of current collector with protective layer:
制备具有保护层的集流体有如下几种方式:There are several ways to prepare a current collector with a protective layer:
(1)先通过气相沉积法或涂布法在绝缘层表面设置保护层,然后通过真空蒸镀、机械辊轧或粘结的方式,在上述具有保护层的绝缘层表面形成一定厚度的导电层本体,以制备具有保护层的集流体(保护层位于绝缘层与导电层本体之间);此外,也可在上述基础上,再在导电层本体的背离绝缘层的面上通过气相沉积法、原位形成法或涂布法形成另外一层保护层,以制备具有保护层的集流体(保护层位于导电层本体的两个相对的表面);(1) First, a protective layer is provided on the surface of the insulating layer by vapor deposition method or coating method, and then a conductive layer of a certain thickness is formed on the surface of the insulating layer with a protective layer by vacuum evaporation, mechanical rolling or bonding. body to prepare a current collector with a protective layer (the protective layer is located between the insulating layer and the conductive layer body); in addition, on the basis of the above, vapor deposition method, In-situ formation method or coating method forms another protective layer to prepare a current collector with protective layer (the protective layer is located on two opposite surfaces of the conductive layer body);
(2)先通过气相沉积法、原位形成法或涂布法在导电层本体的一个表面上形成保护层,然后通过机械辊轧或粘结的方式,将上述具有保护层的导电层本体设置于绝缘层表面,且保护层设置于绝缘层与导电层本体之间,以制备具有保护层的集流体(保护层位于绝缘层与导电层本体之间);此外,也可在上述基础上,再在导电层本体的背离绝缘层的面上通过气相沉积法、原位形成法或涂布法形成另外一层保护层,以制备具有保护层的集流体(保护层位于导电层本体的两个相对的表面);(2) First, a protective layer is formed on one surface of the conductive layer body by a vapor deposition method, an in-situ formation method or a coating method, and then the above-mentioned conductive layer body with a protective layer is arranged by mechanical rolling or bonding. on the surface of the insulating layer, and the protective layer is arranged between the insulating layer and the conductive layer body to prepare a current collector with a protective layer (the protective layer is located between the insulating layer and the conductive layer body); in addition, on the basis of the above, Then another protective layer is formed on the surface of the conductive layer body away from the insulating layer by vapor deposition method, in-situ formation method or coating method to prepare a current collector with a protective layer (the protective layer is located on the two sides of the conductive layer body. opposite surface);
(3)先通过气相沉积法、原位形成法或涂布法在导电层本体的一个表面上形成保护层,然后通过机械辊轧或粘结的方式,将上述具有保护层的导电层本体设置于绝缘层表面,且保护层设置于导电层本体的背离绝缘层的面上,以制备具有保护层的集流体(保护层位于导电层本体的背离绝缘层的表面);(3) First, a protective layer is formed on one surface of the conductive layer body by a vapor deposition method, an in-situ formation method or a coating method, and then the above-mentioned conductive layer body with a protective layer is arranged by mechanical rolling or bonding. on the surface of the insulating layer, and the protective layer is arranged on the surface of the conductive layer body away from the insulating layer to prepare a current collector with a protective layer (the protective layer is located on the surface of the conductive layer body away from the insulating layer);
(4)先通过气相沉积法、原位形成法或涂布法在导电层本体的两个表面上形成保护层,然后通过机械辊轧或粘结的方式,将上述具有保护层的导电层本体设置于绝缘层表面,以制备具有保护层的集流体(保护层位于导电层本体的两个相对的表面);(4) First, a protective layer is formed on both surfaces of the conductive layer body by a vapor deposition method, an in-situ formation method or a coating method, and then the above-mentioned conductive layer body with a protective layer is formed by mechanical rolling or bonding. arranged on the surface of the insulating layer to prepare a current collector with a protective layer (the protective layer is located on two opposite surfaces of the conductive layer body);
(5)在上述“集流体的制备”的基础上,再在导电层本体的背离绝缘层方向的表面上通过气相沉积法、原位形成法或涂布法形成另外一层保护层,以制备具有保护层的集流体(保护层位于导电层本体的背离绝缘层的表面)。(5) On the basis of the above-mentioned "preparation of current collector", another layer of protective layer is formed on the surface of the conductive layer body away from the direction of the insulating layer by vapor deposition method, in-situ formation method or coating method to prepare A current collector with a protective layer (the protective layer is located on the surface of the conductive layer body facing away from the insulating layer).
在制备实施例中,气相沉积法采用真空蒸镀方式,原位形成法采用原位钝化方式,涂布法采用刮刀涂布方式。In the preparation examples, the vapor deposition method adopts the vacuum evaporation method, the in-situ formation method adopts the in-situ passivation method, and the coating method adopts the blade coating method.
真空蒸镀方式的形成条件如下:将经过表面清洁处理的样品置于真空镀室内,以1600℃至2000℃的高温将蒸发室内的保护层材料熔化蒸发,蒸发后的保护层材料经过真空镀室内的冷却系统,最后沉积于样品的表面,形成保护层。The formation conditions of the vacuum evaporation method are as follows: place the surface-cleaned sample in a vacuum coating chamber, melt and evaporate the protective layer material in the evaporation chamber at a high temperature of 1600 ° C to 2000 ° C, and evaporate the protective layer material through the vacuum coating chamber. The cooling system is finally deposited on the surface of the sample to form a protective layer.
原位钝化法的形成条件如下:将导电层本体置于高温氧化环境中,温度控制在160℃至250℃,同时在高温环境中维持氧气供应,处理时间为30min,从而形成金属氧化物类的保护层。The formation conditions of the in-situ passivation method are as follows: the conductive layer body is placed in a high-temperature oxidizing environment, the temperature is controlled at 160 ° C to 250 ° C, and the oxygen supply is maintained in the high temperature environment at the same time, and the processing time is 30 minutes, thereby forming metal oxides protective layer.
凹版涂布方式的形成条件如下:将保护层材料与NMP进行搅拌混合,然后在样品表面涂布上述保护层材料的浆料(固含量为20%~75%),其次用凹版辊控制涂布的厚度,最后在100℃~130℃下进行干燥。The formation conditions of the gravure coating method are as follows: the protective layer material and NMP are stirred and mixed, and then the slurry of the above protective layer material (solid content is 20% to 75%) is coated on the surface of the sample, and then the coating is controlled by a gravure roll. thickness, and finally dried at 100 °C ~ 130 °C.
制备得到的具有保护层的集流体及其极片具体参数如表2所示。The prepared current collector with protective layer and the specific parameters of its pole piece are shown in Table 2.
3、极片的制备:3. Preparation of pole pieces:
通过常规的电池涂布工艺,在集流体的表面涂布正极浆料或负极浆料,100℃干燥后得到正极极片或负极极片。Through a conventional battery coating process, a positive electrode slurry or a negative electrode slurry is coated on the surface of the current collector, and the positive electrode electrode sheet or the negative electrode electrode sheet is obtained after drying at 100°C.
常规正极极片:集流体是厚度为12μm的Al箔片,电极活性材料层是一定厚度的三元(NCM)材料层。Conventional positive electrode: the current collector is an Al foil with a thickness of 12 μm, and the electrode active material layer is a ternary (NCM) material layer with a certain thickness.
常规负极极片:集流体是厚度为8μm的Cu箔片,电极活性材料层是一定厚度的石墨材料层。Conventional negative pole piece: the current collector is a Cu foil with a thickness of 8 μm, and the electrode active material layer is a graphite material layer with a certain thickness.
在表1中,极片1#至极片10#的集流体中没有保护层;在表2中的极片设置有保护层,其中“极片3-1#”表示导电层本体与极片3#的导电层相同,依此类推,“极片6-4#”表示导电层本体与极片6#的导电层相同,依此类推。In Table 1, there is no protective layer in the current collectors from pole piece 1# to
4、电池的制备:4. Preparation of battery:
通过常规的电池制作工艺,将正极极片(压实密度:3.4g/cm3)、PP/PE/PP隔膜和负极极片(压实密度:1.6g/cm3)一起卷绕成裸电芯,然后置入电池壳体中,注入电解液(EC:EMC体积比为3:7,LiPF6为1mol/L),随之进行密封、化成等工序,最终得到锂离子二次电池。Through the conventional battery manufacturing process, the positive electrode (compacted density: 3.4g/cm 3 ), PP/PE/PP separator and negative electrode (compacted density: 1.6 g/cm 3 ) were wound together to form a bare battery The core is then placed in the battery case, and the electrolyte (EC:EMC volume ratio is 3: 7 , LiPF6 is 1mol/L) is injected, followed by sealing, chemical formation and other processes, and finally a lithium ion secondary battery is obtained.
本申请实施例制作的电池以及对比例电池的具体组成如表3所示。Table 3 shows the specific compositions of the batteries prepared in the examples of the present application and the batteries of the comparative example.
表1Table 1
表2:Table 2:
其中,保护层1指位于导电层本体的朝向绝缘层的面(即下表面)上的保护层,其厚度为D3';保护层2指位于导电层本体的背离绝缘层的面(即上表面)上的保护层,其厚度为D3”;“/”代表没有保护层。Among them, the protective layer 1 refers to the protective layer located on the surface of the conductive layer body facing the insulating layer (that is, the lower surface), and its thickness is D3'; the
表3table 3
其中,通过进一步增加电芯的卷绕层数,制备容量得到进一步提高的电池12#和电池13#。Among them, by further increasing the number of winding layers of the battery cells, the battery 12# and the battery 13# with further improved capacity are prepared.
实验例:Experimental example:
1、电池测试方法:1. Battery test method:
对锂离子电池进行循环寿命测试,具体测试方法如下:The cycle life test of lithium-ion battery is carried out, and the specific test method is as follows:
将锂离子电池分别于25℃和45℃两种温度下进行充放电,即先以1C的电流充电至4.2V,然后再以1C的电流放电至2.8V,记录下第一周的放电容量;然后使电池进行1C/1C充放电循环1000周,记录第1000周的电池放电容量,将第1000周的放电容量除以第一周的放电容量,得到第1000周的容量保有率。The lithium-ion battery was charged and discharged at two temperatures of 25°C and 45°C, that is, first charged to 4.2V with a current of 1C, and then discharged to 2.8V with a current of 1C, and recorded the discharge capacity of the first week; The battery was then subjected to 1C/1C charge-discharge cycles for 1000 cycles, the battery discharge capacity at the 1000th cycle was recorded, and the 1000th cycle discharge capacity was divided by the first cycle discharge capacity to obtain the 1000th cycle capacity retention rate.
实验结果如表4所示。The experimental results are shown in Table 4.
2、电池内阻的测试2. Test of battery internal resistance
使用内阻仪(型号为HIOKI-BT3562)进行测试,测试环境为:常温23±2℃。测试前,将内阻仪正负极两端短接校准电阻为零;测试时,将待测锂离子电池进行正负极极耳清洁,然后将内阻仪正负极测试端分别连接到锂离子电池的正负极极耳,进行测试并记录。并根据公式r=A/Cap计算系数A。Use an internal resistance meter (model HIOKI-BT3562) to test, and the test environment is: normal temperature 23±2℃. Before the test, short-circuit the positive and negative ends of the internal resistance meter to calibrate the resistance to zero; during the test, clean the positive and negative electrodes of the lithium-ion battery to be tested, and then connect the positive and negative test ends of the internal resistance meter to the lithium ion battery. The positive and negative tabs of the ion battery are tested and recorded. And calculate the coefficient A according to the formula r=A/Cap.
3、一次穿钉实验和六次连续穿钉实验的实验方法和测试方法:3. Experimental methods and test methods for one nail penetration experiment and six consecutive nail penetration experiments:
(1)一次穿钉实验:电池满充后,固定,在常温下将直径为6mm的钢针,以25mm/s的速度贯穿电池,将钢针保留于电池中,穿钉完毕,然后观察和测试。(1) One nail penetration experiment: After the battery is fully charged, it is fixed. At room temperature, a steel needle with a diameter of 6 mm is passed through the battery at a speed of 25 mm/s, and the steel needle is kept in the battery. test.
(2)六次穿钉实验:电池满充后,固定,在常温下将六根直径为6mm的钢针,以25mm/s的速度先后迅速地贯穿电池,将钢针保留于电池中,穿钉完毕,然后进行观察和测试。(2) Six nail penetration experiments: After the battery is fully charged, it is fixed. At room temperature, six steel needles with a diameter of 6 mm are quickly penetrated through the battery at a speed of 25 mm/s, and the steel needles are retained in the battery. Done, then observe and test.
(3)电池温度的测试:使用多路测温仪,分别于待穿钉的电池的针刺面和背面的几何中心附上感温线,待穿钉完毕后,进行五分钟的电池温度跟踪测试,然后记录下五分钟时的电池的温度。(3) Test of battery temperature: Use a multi-channel thermometer to attach a temperature sensing line to the acupuncture surface and the geometric center of the back of the battery to be pierced. After the piercing is completed, track the battery temperature for five minutes. Test, then record the temperature of the battery for five minutes.
(4)电池电压的测试:将待穿钉的电池的正极和负极连接至内阻仪的测量端,待穿钉完毕后,进行五分钟的电池电压跟踪测试,然后记录下五分钟时的电池的电压。(4) Battery voltage test: Connect the positive and negative electrodes of the battery to be pierced to the measuring end of the internal resistance meter. After the piercing is completed, perform a five-minute battery voltage tracking test, and then record the battery voltage for five minutes. voltage.
记录的电池的温度和电压的数据如表5所示。The recorded battery temperature and voltage data are shown in Table 5.
表4Table 4
表5table 5
注:“N/A”表示一根钢针贯穿入电池瞬间发生热失控和毁坏。Note: "N/A" means that a steel needle penetrates into the battery and thermal runaway and destruction occurs instantaneously.
表6Table 6
根据表4中的结果来看,与采用常规的正极极片和常规的负极极片的电池1#相比,采用本申请实施例集流体的电池的循环寿命良好,与常规的电池的循环性能相当。这说明本申请实施例的集流体并不会对制得的极片和电池有明显的不利影响。尤其是含有保护层的集流体制成的电池,容量保有率进一步获得提升,说明电池的可靠性更好。According to the results in Table 4, compared with the battery 1# using the conventional positive electrode plate and the conventional negative electrode plate, the cycle life of the battery using the current collector of the embodiment of the present application is good, and the cycle performance of the conventional battery is good. quite. This shows that the current collectors in the examples of the present application do not have obvious adverse effects on the prepared pole pieces and batteries. Especially for batteries made of current collectors containing a protective layer, the capacity retention rate is further improved, indicating that the reliability of the batteries is better.
此外,本申请实施例的集流体可以大大改善锂离子电池的安全性能。电池1#和电池4#的电池温度随时间的变化曲线如图22所示,电压随时间的变化曲线如图23所示。从表5以及图22和图23中的结果来看,未采用本申请实施例的集流体的电池1#,在穿钉的瞬间,电池温度骤升几百度,电压骤降至零,这说明在穿钉的瞬间,电池发生内短路,产生大量的热,电池瞬间发生热失控和毁坏,无法继续工作;而且由于在第一根钢针穿入电池之后的瞬间,电池就发生了热失控和毁坏,因此无法对这类电池进行六根钢针连续穿钉实验。In addition, the current collectors of the embodiments of the present application can greatly improve the safety performance of lithium ion batteries. Figure 22 shows the variation curves of battery temperature with time for battery 1# and
而采用了本申请实施例集流体的锂离子电池,尤其是本申请实施例的集流体为正极集流体时,无论对其进行一次穿钉实验还是六次连续穿钉实验,电池温升基本都可以被控制在10℃左右或10℃以下,电压基本保持稳定,电芯可以正常工作。However, the lithium ion battery using the current collector of the embodiment of the present application, especially when the current collector of the embodiment of the present application is the positive electrode current collector, no matter whether it is subjected to one nail penetration experiment or six consecutive nail penetration experiments, the temperature rise of the battery is basically the same. It can be controlled at about 10°C or below 10°C, the voltage is basically stable, and the cells can work normally.
表6中的数据表明,集流体的电阻增大有利于提高电池的内阻r,进而提高系数A值,从而改善电池的安全性能;尤其是当电池的容量较大时,集流体的电阻增大可有效提高电池的内阻r,从而将系数A值保持在较高的数值范围,改善电池的安全性能。The data in Table 6 shows that the increase in the resistance of the current collector is beneficial to increase the internal resistance r of the battery, thereby increasing the value of the coefficient A, thereby improving the safety performance of the battery; especially when the capacity of the battery is large, the resistance of the current collector increases. It can effectively improve the internal resistance r of the battery, so as to keep the value of the coefficient A in a high value range and improve the safety performance of the battery.
可见,在电池发生内短路的情况下,本申请实施例的集流体可极大地降低短路产热量,从而改善电池的安全性能;此外,还可将短路损坏对电池的影响局限于“点”范围,仅形成“点断路”,而不影响电池在短时间内的正常工作。It can be seen that in the case of an internal short circuit in the battery, the current collector of the embodiment of the present application can greatly reduce the short-circuit heat generation, thereby improving the safety performance of the battery; in addition, the impact of the short-circuit damage on the battery can be limited to the "point" range , only a "point break" is formed without affecting the normal operation of the battery in a short period of time.
本申请虽然以较佳实施例公开如上,但并不是用来限定权利要求,任何本领域技术人员在不脱离本申请构思的前提下,都可以做出若干可能的变动和修改,因此本申请的保护范围应当以本申请权利要求所界定的范围为准。Although the present application is disclosed above with preferred embodiments, it is not used to limit the claims. Any person skilled in the art can make some possible changes and modifications without departing from the concept of the present application. The scope of protection shall be subject to the scope defined by the claims of this application.
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| CN201711267487.XA CN109873163B (en) | 2017-12-05 | 2017-12-05 | A current collector, its pole piece and battery and application |
| JP2018152680A JP6858735B2 (en) | 2017-12-05 | 2018-08-14 | Current collectors, their pole sheets, batteries and their applications |
| EP18200693.2A EP3506403B1 (en) | 2017-12-05 | 2018-10-16 | Current collector, electrode plate of the same and battery |
| PT182006932T PT3506403T (en) | 2017-12-05 | 2018-10-16 | Current collector, electrode plate of the same and battery |
| HUE18200693A HUE062079T2 (en) | 2017-12-05 | 2018-10-16 | Current collector, electrode plate of the same and battery |
| US16/209,425 US11024854B2 (en) | 2017-12-05 | 2018-12-04 | Current collector, electrode plate of the same and battery |
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| US20190173089A1 (en) | 2019-06-06 |
| PT3506403T (en) | 2023-05-25 |
| US11024854B2 (en) | 2021-06-01 |
| CN109873163A (en) | 2019-06-11 |
| JP2019102425A (en) | 2019-06-24 |
| HUE062079T2 (en) | 2023-09-28 |
| JP6858735B2 (en) | 2021-04-14 |
| EP3506403A1 (en) | 2019-07-03 |
| EP3506403B1 (en) | 2023-05-10 |
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